Electron beam broadening in electron‐transparent samples at low electron energies

2019 ◽  
Vol 274 (3) ◽  
pp. 150-157 ◽  
Author(s):  
M. HUGENSCHMIDT ◽  
E. MÜLLER ◽  
D. GERTHSEN
1979 ◽  
Vol 16 (6) ◽  
pp. 1680-1685 ◽  
Author(s):  
T. Groves ◽  
D. L. Hammond ◽  
H. Kuo

1997 ◽  
Vol 3 (S2) ◽  
pp. 535-536
Author(s):  
U. Alber ◽  
H. Müllejans ◽  
M. Rühle

Impurity segregation at grain boundaries (GB) can be detected by EDS in a dedicated STEM. Quantification of the segregation requires not only quantification of the spectra but also consideration of the geometry of the experiment. Our aim was to obtain a value which characterises only the segregation of the impurity and is independent of experimental parameters. The problem is that the specimen composition at the GB is extremely inhomogeneous on an atomic scale in the case of Bi segregation at GBs in Cu. The analysed volume which is defined by the irradiated area and the beam broadening of the primary electron beam inside the specimen contains the interfacial plane as well as neighbouring bulk Cu. One approach is to put the focussed primary electron beam on the interface which is aligned edge on and acquire a spectrum. Both the primary beam diameter and the beam broadening inside the specimen have to be known.


1999 ◽  
Vol 5 (S2) ◽  
pp. 292-293
Author(s):  
R. A. Carlton ◽  
C. E. Lyman ◽  
J. E. Roberts

The purpose of this study is to evaluate the variable pressure correction technique (VPCT) as a solution to the problem of extraneous x-ray peaks due to electron beam broadening in the chamber gas of the ESEM. The basis of VPCT is the observation that target x-ray counts decrease with increasing chamber pressure; whereas, x-ray counts due to beam broadening increase. If data are collected at two or more chamber pressures, the number of x-ray counts for an element can be corrected to that expected at zero gas pressure (high vacuum). Tests of NIST SRM 482 have shown EDS x-ray analysis in the ESEM (within the chamber pressure range of 1 to 8 torr) to have comparable accuracy and precision values to those of EDS in the traditional SEM. The samples used in the these studies, however, were quite large (ca. 500 μm in diameter) and so extraneous EDS peaks, due to the electron beam broadening effect of the chamber gas, were minimized.The 60% Au / 40% Cu wire of SRM 482 was pressed into a hole in the surface of an Al specimen stub so as to produce a flat surface with a sharp interface between the wire and the stub. Spectra were collected at 5 and 150 μm from the junction of the wire and the Al stub at chamber pressures of 2, 4, and 8 torr.


Author(s):  
Jong-Shing Bow ◽  
Wei-Chis Lai

Abstract The composition of InGaN/AlN/GaN MQWs nano structure is anlayzed by STEM/EDS. The concentration of nitrogen in GaN materials is usually lower than that of gallium for specimen thickness larger than 50 nm due to low penetration ability of N K X-rays (0.392 KeV). The concentration of indium in the InGaN quanturm wells obtained by STEM/EDS analysis is always much lower its real value. This concentration dilution in this 3 nm structure results from the effect of electron beam broadening, and can be improved to a certain level by reducing specimen thickness, C2 aperture, and dwell time, with a sacrifice in signal intensity.


2001 ◽  
Vol 7 (S2) ◽  
pp. 204-205
Author(s):  
C.-W. Lee ◽  
S. Kidu ◽  
T. Oikawa ◽  
D. Shindo

The electron beam broadening in specimens is a important issue to obtain a high spatial resolution expected by using a fine electron probe of nanometer order in analytical electron microscopy. Beam broadening mainly depends on electron diffusion in specimens. The theoretical equation on the beam broadening, which is based on single scattering approximation model for incident electrons, has been proposed by Goldstein et al.. in this work, the beam broadening was estimated experimentally by a TEM equipped with a field emission gun and the results were compared with the values theoretically obtained.The sizes of the beam diameter with and without specimens were measured by using JEM-2010F and JEM 3000F TEMs, which are equipped with a field emission gun, being operated at 200 and 300 kV, respectively. The beam diameter was defined as the diameter containing 90% of the total electrons. The specimens used were amorphous SiO2, crystalline MgO and Si.


Author(s):  
J. R. Michael ◽  
A. D. Romig

There have been many experimental efforts to measure the spatial resolution for x-ray microanalysis in the analytical electron microscope (AEM). There have been three commonly utilized specimen geometries in these experiments: 1) segregant at a grain boundary, 2) interphase boundaries oriented parallel to the electron beam, and most recently 3) spherical particles embedded at various depths in thin foils. The results of many of these experiments have been analyzed with a number of models for the broadening of the electron beam as it traverses the thin foil. These models are typically based on incoherent electron scattering, typical of Monte Carlo simulations. A vast majority of the published spatial resolution data support the incoherent scattering models as the best simulation of spatial resolution for x-ray microanalysis in the AEM. Recent experimental work using embedded particles to measure beam broadening has been used to support the coherent scattering model of beam broadening.


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